Difference between revisions of "Wave packet"

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:<math> \tilde{\psi}(k) = \frac{1}{\sqrt{2 \pi}} \int {\psi}(x) e^{-i k x } \mathrm{d}x </math>
 
:<math> \tilde{\psi}(k) = \frac{1}{\sqrt{2 \pi}} \int {\psi}(x) e^{-i k x } \mathrm{d}x </math>
 
Note that these two descriptions are [[Fourier transform]]s of one another. Thus, there is an inherent tradeoff between the 'spread' of a wave-packet in position-space vs. momentum-space.
 
Note that these two descriptions are [[Fourier transform]]s of one another. Thus, there is an inherent tradeoff between the 'spread' of a wave-packet in position-space vs. momentum-space.
 
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[[Image:Space tradeoff.png|center|thumb|300px|Tradeoff between spread of a wave-packet in position-space (left) and momenum-space (right).]]
  
 
==Wave-particle duality==
 
==Wave-particle duality==
 
In the context of [[quantum mechanics]], particles can be thought of as wave-packets. That is, quantum particles are neither ideal point-like particles, nor ideal plane-waves. They are instead intermediate objects, which are certainly wave-like (e.g. can undergo interference), but also somewhat localized. The classical concepts of 'particle' (perfectly localized; mathematically a delta-function), and 'wave' (oscillation with a single well-defined wavelength, spread infinitely over all space) can be viewed as limited cases of the general wave-packet. These limiting cases are only conceptual: in reality neither can exist.
 
In the context of [[quantum mechanics]], particles can be thought of as wave-packets. That is, quantum particles are neither ideal point-like particles, nor ideal plane-waves. They are instead intermediate objects, which are certainly wave-like (e.g. can undergo interference), but also somewhat localized. The classical concepts of 'particle' (perfectly localized; mathematically a delta-function), and 'wave' (oscillation with a single well-defined wavelength, spread infinitely over all space) can be viewed as limited cases of the general wave-packet. These limiting cases are only conceptual: in reality neither can exist.
  
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==Components==
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In [[quantum mechanics]], the wave-packet necessarily has both real and imaginary components.
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{|
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| [[Image:Free packet1.png|300px|thumb|Components of the wavefunction (<math>\scriptstyle \psi(x) </math>) describing a propagating wave-packet. The black line is the real part, and the blue line is the imaginary part.]]
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|-
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| [[Image:Free packet2.png|300px|thumb|Square of the wavefunction (<math>\scriptstyle | \psi(x) |^2 </math>) for a  propagating wave-packet. This describes the spatial spread of the function.]]
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|}
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==Propagation and Interaction==
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Wave-packets can propagate, frequently with dispersion (which induces spatial spread of the envelope). Wave-packets can interact with barriers (defined by, e.g., some potential function), and interfere with themselves.
  
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{|
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| [[Image:Wavepacket-Box-wavefunc3.gif|500px|thumb|Components of the wavefunction (<math>\scriptstyle \psi(x) </math>) describing a wave-packet bouncing inside a box-like potential. The black line is the real part, and the blue line is the imaginary part.]]
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|-
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| [[Image:Wavepacket-Box-sqr2.gif|500px|thumb|Square of the wavefunction (<math>\scriptstyle | \psi(x) |^2 </math>) for a wave-packet bouncing inside a box-like potential.]]
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|}
  
 
==See Also==
 
==See Also==
 
* [[Fourier transform]]
 
* [[Fourier transform]]
 
* [http://en.wikipedia.org/wiki/Wave_packet Wikipedia: Wave packet]
 
* [http://en.wikipedia.org/wiki/Wave_packet Wikipedia: Wave packet]

Latest revision as of 08:52, 3 November 2014

A wave packet is a localized wavelike perturbation, which appears frequently in quantum descriptions of particles. For instance, incident x-rays during scattering experiments can be thought of as wave-packets.

A 1D wave packet (with dispersion), propagating over time.
A snapshot of a 2D wave packet.

Position-momentum tradeoff

The wave-packet can be described as a wavefunction in either position-space or momentum-space:

Note that these two descriptions are Fourier transforms of one another. Thus, there is an inherent tradeoff between the 'spread' of a wave-packet in position-space vs. momentum-space.

Tradeoff between spread of a wave-packet in position-space (left) and momenum-space (right).

Wave-particle duality

In the context of quantum mechanics, particles can be thought of as wave-packets. That is, quantum particles are neither ideal point-like particles, nor ideal plane-waves. They are instead intermediate objects, which are certainly wave-like (e.g. can undergo interference), but also somewhat localized. The classical concepts of 'particle' (perfectly localized; mathematically a delta-function), and 'wave' (oscillation with a single well-defined wavelength, spread infinitely over all space) can be viewed as limited cases of the general wave-packet. These limiting cases are only conceptual: in reality neither can exist.

Components

In quantum mechanics, the wave-packet necessarily has both real and imaginary components.

Components of the wavefunction () describing a propagating wave-packet. The black line is the real part, and the blue line is the imaginary part.
Square of the wavefunction () for a propagating wave-packet. This describes the spatial spread of the function.


Propagation and Interaction

Wave-packets can propagate, frequently with dispersion (which induces spatial spread of the envelope). Wave-packets can interact with barriers (defined by, e.g., some potential function), and interfere with themselves.

Components of the wavefunction () describing a wave-packet bouncing inside a box-like potential. The black line is the real part, and the blue line is the imaginary part.
Square of the wavefunction () for a wave-packet bouncing inside a box-like potential.

See Also